2011
DOI: 10.1103/physrevlett.107.048102
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Determination of the Defining Boundary in Nuclear Magnetic Resonance Diffusion Experiments

Abstract: While nuclear magnetic resonance diffusion experiments are widely used to resolve structures confining the diffusion process, it has been elusive whether they can exactly reveal these structures. This question is closely related to x-ray scattering and to Kac's "hear the drum" problem. Although the shape of the drum is not "hearable," we show that the confining boundary of closed pores can indeed be detected using modified Stejskal-Tanner magnetic field gradients that preserve the phase information and enable … Show more

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Cited by 65 publications
(78 citation statements)
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“…In the short mixing time regime, interesting diffusion-diffraction phenomena can be produced [32][33][34][35][36], and angular dependencies can provide insight into pore sizes as shown experimentally first by Koch and Finsterbusch [37,38] and then by others [39][40][41]; however, by analyzing the displacement correlation tensor [42], the short τ m angular DDE experiment aiming to measure compartment sizes was found by Jespersen to be equivalent to a time-dependent SDE experiment [43]. By contrast, in the long mixing time regime, the second order term in the displacement correlation tensor, from which sizes are measured, is decoupled from µA, making its measurement much less complicated [25,31].…”
Section: Introductionmentioning
confidence: 99%
“…In the short mixing time regime, interesting diffusion-diffraction phenomena can be produced [32][33][34][35][36], and angular dependencies can provide insight into pore sizes as shown experimentally first by Koch and Finsterbusch [37,38] and then by others [39][40][41]; however, by analyzing the displacement correlation tensor [42], the short τ m angular DDE experiment aiming to measure compartment sizes was found by Jespersen to be equivalent to a time-dependent SDE experiment [43]. By contrast, in the long mixing time regime, the second order term in the displacement correlation tensor, from which sizes are measured, is decoupled from µA, making its measurement much less complicated [25,31].…”
Section: Introductionmentioning
confidence: 99%
“…1, the molecules will have visited all points inside the pore equally often. Therefore, the time averaged position of each molecule can be approximated to be in the center of mass of the pore space r cm [4]. Thus one arrives at Eðq; 1Þ ¼ expfi2pq Á r cm g S 0 ðqÞ ð 5Þ and, with the above stated limits, the ''long-narrow'' experiment returns the structure factor S 0 ðqÞ directly.…”
Section: Theorymentioning
confidence: 99%
“…In this work we followed the approach of Laun et al where one of the gradients in the standard PGSE NMR experiment is reduced in amplitude and dramatically increased in duration, while the second gradient pulse has to be short and intense [4]. Because of this distinct gradient pattern this experiment has been dubbed ''long-narrow'' PGSE NMR [8].…”
Section: Introductionmentioning
confidence: 98%
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“…Measurement of the diffusive process yields information about a range of properties, including the average propagator for displacement [1,2], the pore space geometry of porous media [3][4][5][6][7][8][9][10][11][12][13], and the characterisation of emulsions [14,15]. Measurement of this process using nuclear magnetic resonance was first described by Hahn [16], with further development and implementation using constant time and pulsed gradient fields by others [17][18][19][20].…”
Section: Introductionmentioning
confidence: 98%